« first day (1400 days earlier)      last day (3916 days later) » 

00:29
Quick check: let $V_n$ be a complex representation of a finite abelian group $G$. Then every element $g \in G$ maps to an operator on $V$ -- and all of these operators are diagonalizable, and share the same set of eigenvectors? Is that last part right? I understand how, by Schur's lemma, V breaks down into 1-dimensional irreducibles. That's the same thing, right?
00:46
Hi @Fernando @Andrew
Heyo Ted
Quiet night on the ranch ....
@FernandoMartin Hey.
sup @Pedro
00:54
@FernandoMartin Remember that Ass M and Supp M exercise with minimal primes?
All we need to assume is minimal primes in Supp M exist right?
I mean, for it to make sense.
01:06
which exercise?
@FernandoMartin That the minimal primes coincide. I think we need A noetherian and M finitely generated.
At least I could prove it under those hypothesis.
yes, those are the ones Matsumura uses
Cool bananas.
I haven't done it yet
Alicia added noetherian
but forgot f.g.
Lel.
http://tabs.ultimate-guitar.com/f/foo_fighters/another_round_crd.htm
D = C9 wtf
Oh, lel.
The text is moved a little.
01:34
@Pedro Let's see if we can do some 'Black Magic' TM to make that equivalence more plausible. So C9 generally has C E G D which we can rearrange with D in the root as D G C E, which I will choose to read as D9sus4
BAM
I have a very 'soft' question for chat. I've heard of the ideas of homotopy and it seems like an active area of research. Can anyone describe how old this field is, how active a field it is, and compare it to other more familiar fields in terms of number of important results?
@fernando some guy wrote vv for the dot product question. half credit
@Kevin what do you mean by "the field of homotopy"? can you be explicit about what you mean?
@MikeMiller You correcting things?
unfortunately yes
What topic?
@MikeMiller I'm not sure I know enough to specify precisely, but the kind of application that would be relevant to me is that idea that we can solve certain easier problem and then somehow continuously deform the solutions to that problem into the solution of some more difficult problem of hte same type
01:42
linear algebra
I guess its not really a field by itself but bundled up in algebraic topology or something
@Kevin the idea of a homotopy between maps is a lot simpler than what could be called homotopy theory in the modem sense, which to my understanding is generally interested in stable homotopy groups of topological spaces, and more abstractly weird category theory stuff
I would guess that what's known as homotopy theory wouldn't be helpful for what you're interested in
@MikeMiller I see, so would you say that the mathematical work that would underlie the kind of application Im talking about has already been done?
I dunno - probably, and what you say sounds like a simple enough idea that you can probably do it ad hoc
@Mike Yeah that was my impression. And I think people do do it ad hoc, but it kinda makes me nervous.
I was kind of hoping that there was still mathematics to be done that might turn out to be really useful for computing solutions of difficult problems
but alas.....
01:50
@Kevin I'm doing something similar (and similarly ad hoc) for a problem of mine; if mainly amounts to keeping careful track of the inequalities involved
@Mike I think my issue is that I wasnt a math major and so I lack a lot of intuition about when things converge and when they converge in the correct space etc etc. My advisor proposed some approximation method for ordinary functions in terms of generalized functions that he'd constructed and it sent me into a tizzy several weeks ago
I didnt know which way way 'up'
02:13
@Kevin You should try reading an intro topology text's chapter on homotopy. Chapter 0 of Hatcher might help you.
@Mike How much background in topology is required? I know the basics but that's about it.
@Kevin Do you know what a continuous map is? Then you're golden.
If you don't like the abstraction it should be pretty easy to restrict to metric spaces in your head.
@Mike a continuous map is one where the pre-image of an open set is an open set?
hope I remember that right
Yes. But if metric spaces are easier for you you lose nothing by thinking in terms of metric spaces, @Kevin
That's good. I don't know anything about non-metric spaces. Everything I work with has a norm.
02:21
A homotopy between $f: X \rightarrow Y$ and $g: X \rightarrow Y$ is a continuous map $X \times I \rightarrow Y$ such that restricting to $X \times 0$ gives you $f$ and restricting to $X \times 1$ gives you $g$
And that's perfectly doable in a metric space!
Yeah it seems so simple but..... like frighteningly so
because there are so many such maps
and its just like 'oh we turn this knob and now we have the solution of a different problem'
just feels os weird to me
03:11
@Kevin But it's not that simple. Not any two maps are homotopic. Do you know about the fundamental group?
@Mike Not really. Something about [0,1] with a boundary and.....
@Kevin Well, as a set, it's homotopy classes of maps from $S^1$ to your pace $X$ (keeping a basepoint fixed in your homotopy). But the point is that this is a useful tool; spaces have lots of non-homotopic maps from $S^1$.
So you can't just go from anything to anything else.
@Mike Yes this makes some kind of sense. If you could do from anything ot anything else it suggests a kind of triviality to what you're looking at. I need to figure out how this applies more concretely
03:26
Hi guys :-)
@Kevin think about loops on the surface of a donut. Can you come up with two that aren't in the same homotopy class? :) (Hint: use the big hole, i.e. the topology of the donut.)
@Kevin So for the application I did I needed all the maps in my homotopy to be "nondegenerate" in a sense and the hard part is figuring out when such a nondegenerate homotopy is actually supported. (Any two of the maps I was considering were homotopic; but they weren't necessarily homotopic in a useful way...)
hi all
But when I could find such a nondegenerate homotopy I could reduce my problem to a trivial case.
hi @mixedmath
how goes it?
03:30
it's alright
I intend to write something for our blog eventually, btw, but I haven't found the time yet
You guys are doing a math blog?
@AndrewG Yep! It just started, and the first post was just put up
Spiffy. I wish I knew enough to do stuff like that.
@AndrewG I guarantee there's a topic you're both passionate and knowledgeable enough about to write on :)
(When I say "our blog", I mean the new Math.SE community blog - open to everyone!)
oh wow
that's an awesome idea
look forward to reading it
03:33
Reset the Net Post this everywhere if you care for your PRIVACY!!!
oh yeah - community blog - anyone and everyone can write!
I thought we weren't resetting the Net until Thursday?
@mixedmath The more people get to join in, the more will be the effect. Everyone doesn't knows of it. So spread the word :)
@mixedmath Do you have a link handy? For a xommunity blog it's hard to find...
@MikeMiller We aren't going to put it on the masthead until it's a bit older and slightly more developed, so right now the only way to know of it is to read meta
@Mike this sounds very similar to what happens in the area of nonlinear dynamics
where each trajectory actually corresponds to a set of trajectories due to some symmerty of the system
and so you need a way of modding out the symmetry to pick exactly 1 representative from each family to find you rpoincare sections
03:39
@mixedmath do you intend to write anything for it?
@MikeMiller I probably will sometime. I'd like it to succeed
@kevin don't frighten me with nonlinear stuff
quadratic is already bad enough
@Mike It scares me too. I do few-body QM. Everything is linear!
@Kevin you should see if you can get a job working on the dynamics of sub linear polynomials
@mixedmath cool, glad to hear it. any idea what on?
something I've been thinking a lot about recently is pretty data visualization with matplotlib, actually
03:45
@Mike sub....linear...polynomial......WAT!?
pretty things have wide appeal!
@Kevin I hear they behave particularly nicely :)
so one thing might be to just look at data about MSE and present it nicely and explicitly
those.....those just sounds like constants @Mike
;)
@mixedmath by the way, you wrote me a long email a while back about life at Brown - I ended up accepting an offer somewhere else, but I want to say again I really appreciate it!
@MikeMiller oh yeah, that's right. So where are you going?
03:53
Did @mixedmath go to Brown?
@KevinDriscoll I'm there now. I'm a 4th year grad student
At Duke, Brown was always the ivy that we picked on. It frequently gets called 'clown college.'
Howdy @Kevin @Mike @mixed ....
Ah okay. Grad program.... totally unrelated.
Hi @TedShifrin
03:53
@Ted howdy
Hi @Ted
Hi @nabla
@mixedmath I'll be heading to UCLA in the fall
hi @TedShifrin
@MikeMiller Way cool. There's some good number theory there (and I'm all about the number theory)
@mixedmath Lots of good stuff all around. Glad to be heading there!
@Ted Too many margaritas?
03:57
No, iPad typo. No booze whatsoever :(
Too few margaritas, then
Ive never understood the widespread love of margaritas
I think tequila is nasty
Also, I'm hardcore procrastinating on writing my thesis proposal
I'm a gin fanatic, but many dislike that, too. :) At the moment I'm trying to lose weight, so have cut back on booze.
@Kevin: Imagine how much you'll procrastinate on the real thing.
Margaritas + seafood = win. Tis a theorem.
04:06
@Ted I've decided that the major obstacle to every PhD is the students fight with his own self-motivation
external factors are oftne neglegible
Not if it's French or Italian food, as opposed to Mexican @Andrew
Also< i quite like gin
@Ted Killing time with gin and lime?
I was very motivated in grad school, but hit plenty of brick walls regardless.
Successive approximations @Mike?
Is there a well-known tiering list for schools int erms of math faculty positions? I hear people talking about tier 2 and tier 3 schools and I wonder where the 'official list' is
04:08
@TedShifrin Yes, I suppose in that case a good wine would be the necessary condition.
There are AMS rankings, mostly based on department heads' opinions, which are often biased and way dated.
@Ted well rats you've disproved my hypothesis
Okay, so its very similar to how physics works. I really dislike this system. What happens is the department head says 'who do I know from X?' and their knowledge is of course skewed toward hteir field
Well, USNews gets the top 5 right. Not necessarily in order.
so they artifically rank schools lower/higher based on a single field
at leas thtats how it usually works for us
How do they do it? @Mike
I'm not sure any of us have an order. The order is random and/or field-dependent if there is one.
04:11
@Ted I don't remember how they order them but their top 5 is MIT, Stanford, Berkeley, Princeton, Harvard
Ah, Stanford has replaced Chicago?
If they do it like their undergrad rankings its a compound thing. Part is survey of department heads. part is post-grad survey. Part is work outcomes of students. Part is number of publications and what journals theyre in.....
Otherwise, the list hasn't changed in 30 years.
I use ARWU
Man I don't care about the top 5 at this point. I'll take a tenure track position at a small/medium sized state school and be quite happy. Thank you very much.
04:13
@Ted They might have it all as a top 6 now with Chicago tied in there, but maybe not.
I am surprised Stanford is that high, but it's not silly. Chicago is no longer what it was in the 60s.
It doesn't help that any such list is necessarily going to resist change
I think the top 6 for physics is identical
although you also nee dto include Cal tech
I think those are generally just six of the best funded, most renowned universities I'm the nation, so you'll probably see the "top 5" for most fields in general just be 5 of some set of 10 schools.
Morning..
04:17
Ah, done slumbering, @Studentmath?
Yeah, it flows well once again
No idea what I had, was so odd, everything went wrong :P
LOL ... Not a catastrophe, nor a dogmatic failure. :)
Fortunately - or rather hopefully :)
hey @Ted, random topology question. Suppose I wanted to construct a surface, embeddable in $\mathbb{R}^3$, with fundamental group $\mathbb{Z}_2$. Only thing I can think of is the real projective plane but that's not embeddable.
Every compact surface without boundary in $\Bbb R^3$ must be orientable.
Can't happen, by classification of surfaces. @Mike can crank universal coeff theorems:
04:21
So it's not possible
K
Also seems what I thought to be conditional yesterday is actually multipication
Here is the inequality I told you about
Multiplication? @Studentmath ... You mean "and"?
Get back to me when I'm teaching probability in a few months :)
04:25
let $n$ be a positive integer and let $a_1,a_2\dots a_n\in \mathbb R$ with $a_1+a_2\dots a_k\leq k$ for $k=1,2\dots n$ prove $\frac{a_1}{1}+\frac{a_2}{2}\dots\frac{a_n}{n}\leq \frac{1}{1}+\frac{1}{2}\dots \frac{1}{n}$
The probability of $Y_{(1)}<3Y_{(2)}$ requires two simultaneous conditions
When will that be?
Ok, night, all ...
@TedShifrin It's obviously not the case for closed surfaces by classification. The question for non-closed surfaces isn't obvious to me, though don't spoil it.
Later @Ted
Later Professor
04:26
Good night Prof. @Ted
@skullpatrol Hi.
I love this place. Ask a question, and you get plenty to google and read about.
I think I might have an answer @AndrewG but it's probably needlessly high-powered... let me fiddle with it a little more
This chat was made as a battfield to test the effects of nuclear mathematics on mosquito sized problems
4
nope, argument doesn't work.
04:40
Darn :| what were you trying though? curious but probably won't understand
I've never taken topology beyond point-set, so I'm reading about classification of surfaces right now.
Classification of surfaces is awesome! It's one of the things that convinced me combinatorics wasn't so bad after all, since it's essentially a combinatorial argument.
@AndrewG I wanted to start with a surface embedded into $S^3$ and use Alexander duality to show that its complement would have first homology = $\mathbb Z_2$ (this is the first place it fails) and then say that the complement would be an open subset of $S^3$ (also not true) and then that the first homology of an orientable manifold has no torsion in $H_1$ (also not true).
So I wanted to use one bogus argument and three false facts.
@MikeMiller That's the best way to prove things, though.
Yep, way over my head, but more to look up, at least.
Haha if you removed your admissions that these things are untrue you couldve successfully pulled off a proof by intimidation
Anyway, one can have closed orientable manifolds that have fundamental group $\mathbb Z_2$. They just can't embed into $\mathbb R^3$.
I just don't know how to show they can't embed into $\mathbb R^3$ yet :p
04:55
Is there a way to put a cross on something written on the forums?
I.e. a line through
There's no markdown for it, but the HTML tags are allowed, like <strike>this</strike> or <s>this</s> or <del>this</del>
371
Q: What HTML tags are allowed on Stack Exchange sites?

Jeff AtwoodThe Stack Overflow site engine, as you know, uses Markdown for questions and answers. Per the Markdown spec, you are allowed to freely intermix HTML and Markdown tags. Not all HTML tags are allowed, as that would be an XSS paradise. Which HTML tags have been whitelisted and are allowed to be use...

@AndrewG to prove Ted's assertion: by classification of surfaces, $\mathbb{RP}^2$ is the only compact surface without boundary with fundamental group $\mathbb Z_2$. (see this by representing every surface as a quotient of a polygon.) so one only needs to show $\mathbb{RP}^2$ can't embed in $\mathbb R^3$, which can be done with alexander duality
representing a surface by a polygon = generalization of building a torus by modding the plane by a lattice, etc?
identifying sides and so-on?
Thanks @David, eventually just deleted it..
05:06
@AndrewG page 5
ah k
I still don't get that question though..
sigh statistics
@Studentmath, same question from last night regarding distributions?
Does he have a section on Alexander duality? I don't see it in the table of contents.
Not sure which one you speak of - the one regarding ordered statistics. I managed the other one with Gamma Distribution, went out nicely
05:10
Ah, awesome, yeah I was wondering about the Gamma distribution.. Glad to hear that you got it figured out
This oddie one now:
http://math.stackexchange.com/questions/819269/probability-that-order-statistic-is-larger-than-the-other
Yeah, I was over-complicating it. Should've just went straight on with the gut feeling, reasonable explanations and statements and you can use the gamma distribution to finish it off nicely :)
Also, I'm wondering now if there might be some crazy Seifert surface with the right properties.
At least I went from not understanding it to understanding it yet failing to solve
@Student, yeah, it seemed to me that you had figured it out but hadn't yet settled on an interpretation.
@AndrewG It's at the veeeery end of chapter 3. It says, in particular, that $\tilde H_0(S^3 \setminus \mathbb{RP}^2, \mathbb Z) \cong H^2(\mathbb{RP}^2, \mathbb Z)$; but the first thing is always free abelian, and the second thing is $\mathbb Z_2$, which is a contradiction.
05:20
Nice.
I feel like it should be easier. (There's almost certainly an easier way to do it if you want your embedding to be smooth.)
Is this a typical use of (co)homology groups? I've never really understood why one should bother with them, but showing that one space is not embeddable in another seems like a pretty practical thing.
@David Baby-steps. It's considered a tough question, hence my focus on it
I think I better back up and read this whole chapter :|
@AndrewG (co)homology is incredibly useful! Some things you might like, that I know how to do most easily with them: $\mathbb R^m \cong \mathbb R^n$ iff $m=n$; every map from the closed unit ball to itself has a fixed point; no compact manifold retracts onto its boundary; the Euler characteristic of any manifold of odd dimension is 0.
05:33
@Student, you are wise to look deeper. it's an important question -- one that gets asked in different ways by countless disciplines.
Is it possible to derive cauchy schwarz on $\Bbb R^n$ as a consequence of the triangle inequality?
Okay that was silly, of course $A'$ has a fixed point. Ignore me.
Awww lol
My topology professor gave me that as an exercise, and I just realized it's trivial! He's got hell to pay, @AndrewG
05:38
I was still reading it when you yoinked it, so I dunno what it was exactly or how it was trivial :P but the Lefschetz fixed-point theorem does look awesome.
@AndrewG Because $A(0) = 0$...
Hi pal @Parth Kohli
Oh, haha, yes.
This Lefschetz thing is crazy.
@AndrewG Chapter 2 of Hatcher doesn't require anything from chapter 1, so if you're interested in this, that's a good place to start. (Read chapter 0 first, though.)
There's so much beautiful math to learn :O
05:45
yase
@AndrewG If it's beautiful, it's not math.
how wrong you are
(Joke.)
@AndrewG I did some googling, and it turns out that the fundamental group of any submanifold of $S^3$ is torsion-free... but it seems like it uses a lot of really hard stuff I don't know about yet.
Nevermind, it says any submanifold with connected complement.
@MikeMiller OK, so, I take a surface, cut it up and lay it out as a polygon, triangulate it, and start calculating the simplicial homology. I've seen this before (a bit) but should practice doing it. One thing, though: there are dozens of homology and cohomology theories, right? But I've often heard of "the" homology/cohomology of a space, as if they're all equivalent? Do all roads lead to Rome or something?
Also, that's cool, at least you're narrowing down the possibilities lol
06:00
@AndrewG Yes, there are lots, but don't get lost in that right now. They don't necessarily even have to do with topological spaces. The ones you'll learn from Hatcher are called simplicial homology, singular (co)homology, and cellular homology... and those three are the same whenever they're both defined.
When one says the homology of a space they mean the singular homology unless otherwise specified.
To clarify: simplicial/singular/cellular homology are all the same (on spaces where they're defined). Singular homology and singular cohomology are very different.
Right. But they have dualities relating them.
I've heard of Poincare duality but don't really know what it is except it relates those.
For manifolds there are dualities relating them.
06:03
As groups, cohomology is entirely determined from homology by the Universal Coefficient Theorem. Despite that, cohomology has a lot of its own stuff to say that homology doesn't.
Cool
In particular, cohomology has a natural ring structure in addition to the group structure - and that ring structure can tell spaces apart that the group structure can't
So non-isomorphic spaces can have the same homology groups, but the cohomology groups can distinguish them through that extra info?
Sure. (Not necessarily, though. For instance, neither homology nor cohomology can tell the Mobius strip apart from the cylinder - both are homotopy equivalent to the circle, and both homology and cohomology - including the ring structure - are homotopy invariants.)
As I understand it, the fundamental meaning of cohomology is to be found in differential forms, which you can think of as the thing you integrate when doing a line integral (for my example, e.g. Pdx + Qdy say). Think of R^n with a hole at the origin, how do we detect it? We only have functions that are defined inside the space, if we go off to zero we don't know we're going to a hole at the origin, so we need some way to test for it.
All we know is that line integrals depend only on their endpoints for nice functions, so we try to find a differential form that, when we integrate it (in, say, a circle), we do not end up with zero. This means we went around a hole in the space. Furthermore, we know that integrals of crazy paths around the hole will give the same values as circles, and also that a load of different functions will give non-zero values as we go around the hole, so we need a way to simplify working with all these things... Based on this simple geometric picture, illustrated here:
we see that all that crazy algebra, group theory, ring theory etc... falls upon us naturally when we try to group all the differential forms with these properties into sets. You have to categorize the set of forms into equivalence classes using the only tools you have, the exterior derivative operator, and because this operator has some freedom in it you end up with group structure and all this stuff
http://en.wikipedia.org/wiki/De_Rham_cohomology
Hopefully that will give some geometric intuition and motivation behind the crazy algebra definitions
Maybe there's a better way to think about it, but the only other way I've seen is unmotivated algebra which I'm too stupid to understand :p
@MikeMiller how does one tell them apart? The only way I've seen is using fiber bundles, is there a way using homology or homotopy?
06:24
@bolbteppa One is orientable, the other is not (and orientable can be defined completely homologically). but that's probably what you mean by "using fiber bundles".
Yeah, I don't understand differential forms well enough yet for deRham cohomology
Maybe soon
That's cool though
@AndrewG if you read the link I gave you, and read the paper I linked to in that article, you'll understand differential forms very quickly, and with lovely pictures :p The idea is that a differential form sets up a field of sheets, and integrating a differential form along a curve is just a way of counting how many sheets the curve passes through.
@bolbteppa You're new around these parts (or at least new to me). What's your story?
@MikeMiller am I understanding right that the original question is still open, so long as the manifold has a boundary and its complement is disconnected? lol
That explains why line integrals are path-independent, depend on end-points, closed-loops give zero etc... (all those theorems in multivariable calculus), you just go forward through the sheets then back against them so you ultimately go through no sheets... Sometimes though, the field of sheets all spring out from one point and give a cone/fan shape which represents a singularity (see the answer to my question in that post), so when you go around in a circle you go around 2pi's worth of sheets
06:30
@AndrewG i'm sure one can answer it from existing theorems, but I don't know the answer.
Well I'm certainly finding a lot to learn along the way, which is really better anyways.
My story right now is that it's 7am, I've been awake for a day, and I have to now go and read a paper on the Ising Model and Algebraic Bethe Ansatz's work for quantum integrable models, all the while barely knowing elliptic integrals or how to geometrically derive ellipsoidal coordinates :p What's yours?
it's 2:34 am, woke up at 11 pm and brewed a pot of coffee -- supposed to be writing software but procrastinating and playing with math instead.
Yeah I am supposed to learn mathematica on top of all this, keep getting distracted by math and coffee too
Do you think mathematica is the kind of thing you can pick up in about 2 hours, or is it insanely complicated?
eh, well ... you can do basic symbolic manipulation right out of the gate, but anything remotely non-trivial is going to hang your computer processor ;)
06:37
@MikeMiller what's it mean to say that a manifold is torsion-free? that its fundamental group has no elements of finite order?
Great stuff
In differential geometry, the notion of torsion is a manner of characterizing a twist or screw of a moving frame around a curve. The torsion of a curve, as it appears in the Frenet–Serret formulas, for instance, quantifies the twist of a curve about its tangent vector as the curve evolves (or rather the rotation of the Frenet–Serret frame about the tangent vector). In the geometry of surfaces, the geodesic torsion describes how a surface twists about a curve on the surface. The companion notion of curvature measures how moving frames "roll" along a curve "without twisting". More gener...
Oh, sorry, I misread you earlier: you said the fundamental group was torsion-free. Nevermind.
I need more coffee.
good idea... (off to grab a cup and a smoke)
07:20
Hullo @bolbteppa
07:38
So, I bought Kolmogorov and Fomin used through Amazon. And apparently it used to belong to some lady professor. And she put a Hello Kitty sticker inside the front. I don't know why, but this makes me happy.
Bought?
It's not the same if you can't hold it in your hand.
@AndrewG Nonsense. I heard many people say that. I find no difference between holding and reading from the computer.
To each his own :P if one is just as good as the other for you, so be it. I can't get enough of paper.
Besides, you can't put Hello Kitty stickers inside the covers of PDF files. That alone is reason to buy books!
My fundamental reason to get PDF files is to prevent someone putting stickers in the math books.
07:46
Party pooper.
Someday, you'll find books that is not available in hard copy anywhere. Someday.
When that day comes, I will find a PDF of it, print it out, bind it myself, and put a Hello Kitty sticker in it, just to annoy you. :P
@MikeMiller am I correct in the following understanding? Trying to get the point of relative homology groups and all this diagram chasing/homological algebra in Ch. 2. So, take for example the Klein four-group v.s. the cyclic group $\mathbb{Z}_4$. They both contain $\mathbb{Z}_2$ and quotient to $\mathbb{Z}_2$. I can represent both of these situations with a short exact sequence. If, however, I just decided to extend $Z_2$ by $Z_2$, there are two ways to do it. I have to decide which one.
@MikeMiller am I understanding correctly that all this diagram chasing stuff is just a fancy way of picking the 'right' extension?
sigh I never studied homology, even though I want to read it.
08:02
@BalarkaSen It looks pretty cool. Mike has me reading Hatcher :)
@AndrewG Yeah, someone recommended me that for homotopy instead.
I like homotopy, even though I am just scratching the surface with covering space stuffs.
Hi folks
Any clue would be appreciated, specially something with extreme validity!
@BalarkaSen @robjohn @nablablah @skullpatrol (With respect)
You're applying $x = \sin(\theta)$. But that restricts the whole domain $D$ (indefinite) to the some bounded domain $[0, 1]$, @MrWho.
@BalarkaSen Well, how does it affect the final answer to the integral?
@BalarkaSen If you give me mathematical step by step reason for my question I absolutely understand what you mean then.
@MrWho My guess is that it takes up the "remains" and adds it to the constant term, i.e., pick up all the $x$ which is not in $[0, 1]$ and integrate up. I am not sure though, this is just a wild guess.
08:20
@BalarkaSen I think my question is asking about something happening in the back-end of the method, very nature of this technique, just looking for robust answer.
@MrWho Yes, that's why I am saying it has something to do with the "crumpling" of the domain through that u-sub.
@BalarkaSen Seriously, I myself don't really know anything about the effects of domain movement via substitution, anyway, I stay tuned looking for an answer.
Both of the answers seem to take the question to he theoretical level, instead of looking at the method, sadly.
@BalarkaSen Yeah :(
08:23
Shame he shown no effort
@MrWho Maybe you should make it clear what you're asking.
@BalarkaSen The answer is yes, it seems I didn't drive my question to the right destination!
@BalarkaSen Surprisingly, you are the only one who understood it!they think I don't know the constant would be the constant and there is infinite answer for the integral.
@MrWho I have - forgive me - an ability to think out of the box, yes, I wouldn't deny that.
At least we can call @robjohn. @robjohn Do you see what's intended to be asked?
@BalarkaSen Help me! I don't really know how to paraphrase the question, seriously, I think I crafted the question in the artistic way!
08:31
@MrWho As for that, I am not sure either how to get the question in the right track, sorry.
@BalarkaSen You see, I don't ask lots of questions, and even if I ask one (once in a season) the question would be convicted to be completely vague or intractable to be controlled!
@robjohn @BalarkaSen Well, why would $\frac {-1}{4}$ rise up when we use the trigonometric substitution rather than the general formula?For the sake of god,DO NOT remind me that constants are the same, and I certainly know that $\frac {-1}{4}$ is the part of the constants which can be applied to the question.But why $\frac {-1}{4}$ would be detached from the general constant and join the integration answer?
@MrWho You might want to edit our question. Someone changed that $\sin(2\theta)$s into $\sin^2(\theta)$, making it confusing.
@robjohn @BalarkaSen Why $C$ which I call it the general constant is converted to $C'+\frac {-1}{4}$ when trig sub is applied? (The simplest way to represent what I mean) - Sorry for calling you guys several times.
r9m
r9m
@Sawarnik AH ... thanks a lot !! ;) :D
08:46
@BalarkaSen Ah, I see, clumsy editor, damn it!
@MrWho two anti-derivatives are equivalent if they differ by a constant. This is the purpose of the constant of integration, to account for this fact.
@robjohn I believe he much wants to know in which step $-1/4$ comes into play. Can you kindly point that out?
@robjohn I know what you've just said and my question is not asking anything about this fact.
If the constant of integration were going to be the same, we wouldn't need to leave it as $C$, we could simply leave it as $13$, or whatever.
@BalarkaSen Your last statement is what I mean :|
08:50
@MrWho let's keep our temper a little down, ok? and pinpoint what we want to know to @robjohn.
@BalarkaSen $\frac{\mathrm{d}}{\mathrm{d}x}\left(-\frac14\right)=0$
@robjohn That is understood. But I think what @MrWho wants to know is where does it appear in his derivation. My guess is that there is some domain inconsistency when applying the sub $x = \sin(\theta)$, i suspect this is the root of the problem.
But it's likely I am mistaken
@robjohn @BalarkaSen Why $\frac {-1}{4}$ show itself when we use trigonometric substitution instead of general formual?I know it won't hurt integration answer but why is $\frac {-1}{4}$ detached?
@MrWho This is simply an artifact of the method of integration. As you say, it does not affect the answer. One constant of integration is as good as any other.
@robjohn With all due respect, I humbly disagree with you.There must be a clue to clarify the transpiration of the artifact you spot to.
@BalarkaSen @robjohn By mentioning artifact we're just escaping from finding the rationale behind it.
08:58
@MrWho How are you getting this equality? : $$\dfrac{-1}{4}(\cos^2\theta-\sin^2\theta)+C=\dfrac{-1}{4}+(\dfrac{-1}{4}+\frac{‌​x^2}{2})+C'$$
@BalarkaSen I'm not getting this?!
@BalarkaSen Think that the editor ruined my question!
That's what is written in the question.
@BalarkaSen Editor! :(

« first day (1400 days earlier)      last day (3916 days later) »